Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





Chosen Fixed Point

Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
55606 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{5}^{2}$ 0.6106 0.7803 0.7826 [M:[1.2857, 0.9107, 0.7143, 0.8036, 1.0, 0.7143], q:[0.4018, 0.3125], qb:[0.6875, 0.8839], phi:[0.4286]] [M:[[0], [2], [0], [-2], [0], [0]], q:[[-1], [1]], qb:[[-1], [1]], phi:[[0]]] 1 {a: 53619/87808, c: 68515/87808, M1: 9/7, M2: 51/56, M3: 5/7, M4: 45/56, M5: 1, M6: 5/7, q1: 45/112, q2: 5/16, qb1: 11/16, qb2: 99/112, phi1: 3/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{6}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}q_{1}q_{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}q_{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$ ${}\phi_{1}^{3}q_{1}q_{2}$ -1 2*t^2.143 + t^2.411 + t^2.571 + t^2.732 + t^3. + t^3.161 + t^3.429 + t^3.696 + 3*t^4.286 + 2*t^4.554 + 3*t^4.714 + t^4.821 + 2*t^4.875 + t^4.982 + 4*t^5.143 + 3*t^5.304 + t^5.411 + t^5.464 + 3*t^5.571 + t^5.732 + 2*t^5.839 + t^5.893 - t^6. + t^6.107 + t^6.161 + t^6.321 + 4*t^6.429 + 3*t^6.696 + 3*t^6.857 + 2*t^6.964 + t^7.018 + 2*t^7.125 + t^7.232 + 5*t^7.286 + 2*t^7.393 + 5*t^7.446 + 3*t^7.554 + 2*t^7.607 + 6*t^7.714 + t^7.821 + 4*t^7.875 + 3*t^7.982 + 3*t^8.036 - 2*t^8.143 + t^8.196 + 2*t^8.25 + 2*t^8.304 - 2*t^8.411 + 3*t^8.464 + t^8.518 + 3*t^8.571 + t^8.625 - 2*t^8.732 + 3*t^8.839 + t^8.893 - t^4.286/y - t^6.429/y - t^6.696/y - t^6.857/y - t^7.018/y + t^7.286/y + (3*t^7.554)/y + (3*t^7.714)/y + (3*t^7.875)/y + t^7.982/y + (4*t^8.143)/y + (3*t^8.304)/y + t^8.411/y + (3*t^8.571)/y + (2*t^8.732)/y + (2*t^8.839)/y + t^8.893/y - t^4.286*y - t^6.429*y - t^6.696*y - t^6.857*y - t^7.018*y + t^7.286*y + 3*t^7.554*y + 3*t^7.714*y + 3*t^7.875*y + t^7.982*y + 4*t^8.143*y + 3*t^8.304*y + t^8.411*y + 3*t^8.571*y + 2*t^8.732*y + 2*t^8.839*y + t^8.893*y 2*t^2.143 + t^2.411/g1^2 + t^2.571 + g1^2*t^2.732 + t^3. + g1^2*t^3.161 + t^3.429 + t^3.696/g1^2 + 3*t^4.286 + (2*t^4.554)/g1^2 + 3*t^4.714 + t^4.821/g1^4 + 2*g1^2*t^4.875 + t^4.982/g1^2 + 4*t^5.143 + 3*g1^2*t^5.304 + t^5.411/g1^2 + g1^4*t^5.464 + 3*t^5.571 + g1^2*t^5.732 + (2*t^5.839)/g1^2 + g1^4*t^5.893 - t^6. + t^6.107/g1^4 + g1^2*t^6.161 + g1^4*t^6.321 + 4*t^6.429 + (3*t^6.696)/g1^2 + 3*t^6.857 + (2*t^6.964)/g1^4 + g1^2*t^7.018 + (2*t^7.125)/g1^2 + t^7.232/g1^6 + 5*t^7.286 + (2*t^7.393)/g1^4 + 5*g1^2*t^7.446 + (3*t^7.554)/g1^2 + 2*g1^4*t^7.607 + 6*t^7.714 + t^7.821/g1^4 + 4*g1^2*t^7.875 + (3*t^7.982)/g1^2 + 3*g1^4*t^8.036 - 2*t^8.143 + g1^6*t^8.196 + (2*t^8.25)/g1^4 + 2*g1^2*t^8.304 - (2*t^8.411)/g1^2 + 3*g1^4*t^8.464 + t^8.518/g1^6 + 3*t^8.571 + g1^6*t^8.625 - 2*g1^2*t^8.732 + (3*t^8.839)/g1^2 + g1^4*t^8.893 - t^4.286/y - t^6.429/y - t^6.696/(g1^2*y) - t^6.857/y - (g1^2*t^7.018)/y + t^7.286/y + (3*t^7.554)/(g1^2*y) + (3*t^7.714)/y + (3*g1^2*t^7.875)/y + t^7.982/(g1^2*y) + (4*t^8.143)/y + (3*g1^2*t^8.304)/y + t^8.411/(g1^2*y) + (3*t^8.571)/y + (2*g1^2*t^8.732)/y + (2*t^8.839)/(g1^2*y) + (g1^4*t^8.893)/y - t^4.286*y - t^6.429*y - (t^6.696*y)/g1^2 - t^6.857*y - g1^2*t^7.018*y + t^7.286*y + (3*t^7.554*y)/g1^2 + 3*t^7.714*y + 3*g1^2*t^7.875*y + (t^7.982*y)/g1^2 + 4*t^8.143*y + 3*g1^2*t^8.304*y + (t^8.411*y)/g1^2 + 3*t^8.571*y + 2*g1^2*t^8.732*y + (2*t^8.839*y)/g1^2 + g1^4*t^8.893*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
57253 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{5}^{2}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ 0.6294 0.8148 0.7724 [M:[1.2857, 0.8901, 0.7143, 0.8242, 1.0, 0.7143, 0.7472], q:[0.4121, 0.3022], qb:[0.6978, 0.8736], phi:[0.4286]] 2*t^2.143 + t^2.242 + t^2.473 + t^2.571 + t^2.67 + t^3. + t^3.099 + t^3.429 + 3*t^4.286 + 2*t^4.384 + t^4.483 + 2*t^4.616 + 4*t^4.714 + 3*t^4.813 + t^4.912 + t^4.945 + t^5.044 + 4*t^5.143 + 4*t^5.242 + 2*t^5.34 + t^5.473 + 3*t^5.571 + 2*t^5.67 + t^5.769 - t^6. - t^4.286/y - t^4.286*y detail


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from the Same Seed Theory

Below is a list of equivalent fixed points from the same seed theories.

id Theory Superpotential Central Charge $a$ Central Charge $c$ Ratio $a/c$ $R$-charges More Info. Rational


Previous Theory

The previous fixed point before deforming to get the chosen fixed point.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
47176 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ 0.6706 0.8484 0.7904 [M:[1.1549, 0.7464, 0.8451, 0.7935, 0.6948, 0.8451], q:[0.3967, 0.4484], qb:[0.8569, 0.7582], phi:[0.385]] t^2.084 + t^2.239 + t^2.31 + t^2.38 + 2*t^2.535 + t^3.535 + t^3.69 + t^3.845 + t^4.169 + t^4.324 + t^4.394 + t^4.465 + t^4.478 + t^4.549 + 4*t^4.62 + t^4.69 + t^4.761 + 2*t^4.775 + 3*t^4.845 + 2*t^4.916 + 3*t^5.071 + t^5.62 + t^5.775 + t^5.916 + t^5.929 - 2*t^6. - t^4.155/y - t^4.155*y detail